A guarded parallel‐plate instrument for measuring the thermal conductivity of fluids in the critical region

1989 ◽  
Vol 60 (11) ◽  
pp. 3466-3474 ◽  
Author(s):  
R. Mostert ◽  
H. R. van den Berg ◽  
P. S. van der Gulik
Author(s):  
Milivoje M. Kostic ◽  
Casey J. Walleck

A steady-state, parallel-plate thermal conductivity (PPTC) apparatus has been developed and used for comparative measurements of complex POLY-nanofluids, in order to compare results with the corresponding measurements using the transient, hotwire thermal conductivity (HWTC) apparatus. The related measurements in the literature, mostly with HWTC method, have been inconsistent and with measured thermal conductivities far beyond prediction using the well-known mixture theory. The objective was to check out if existing and well-established HWTC method might have some unknown issues while measuring TC of complex nano-mixture suspensions, like electro-magnetic phenomena, undetectable hot-wire vibrations, and others. These initial and limited measurements have shown considerable difference between the two methods, where the TC enhancements measured with PPTC apparatus were about three times smaller than with HWTC apparatus, the former data being much closer to the mixture theory prediction. However, the influence of measurement method is not conclusive since it has been observed that the complex nano-mixture suspensions were very unstable during the lengthy steady-state measurements as compared to rather quick transient HWTC method. The nanofluid suspension instability might be the main reason for very inconsistent results in the literature. It is necessary to expend investigation with more stable nano-mixture suspensions.


1996 ◽  
Vol 105 (23) ◽  
pp. 10535-10555 ◽  
Author(s):  
E. P. Sakonidou ◽  
H. R. van den Berg ◽  
C. A. ten Seldam ◽  
J. V. Sengers

When Miss Nelson and the writer prepared in 1929 an article for the 'International Critical Tables' on the thermal conductivity of gases, we found that the value for air had been measured by 19 observers and that the mean departure from the mean was 7%. Further the values obtained by the hot wire method by Weber, Gregory and Archer, and Schneider were higher than the value (5.40 X 10 -5 cal. cm. -1 sec. -1 deg. -1 ) which Hercus and the writer had found by a parallel plate method, and higher than 13 of the 14 determinations (including hot wire ones) made previous to 1918. In view of these facts it was desirable to repeat the parallel plate method and to obtain evidence as to whether or not there was a systematic difference between the two methods mentioned. The hot wire method, as used by the experimenters named, has the practical advantages measured, and it is convenient and simple. As carried out in the experiments referred to in which fine wires were used it has the disadvantages that the elimination of the convection effects is not attained with certainly, the temperature gradient in the gas is large (which introduces both theoretical and practical difficulties) and there is a temperature discontinuity at the surface of the wire which has to be determined. Hercus and Sutherland have nearly completed in this laboratory a measurement of the thermal conductivity of air with a parallel plate apparatus. This method has the inherent advantages that there are no convection currents in the horizontal lamina of gas used, that the temperature gradient may be made small, and the temperature disments now in progress radiation is eliminated by using the metal plates at two different separations and considerable improvements have been made us compared with the experiment of Hercus and in their measurement.


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